Electric field: Difference between revisions
No edit summary |
|||
(10 intermediate revisions by 2 users not shown) | |||
Line 1: | Line 1: | ||
====Electric field==== | ====Electric field==== | ||
Claimed by David Gamero (Fall 2016) | |||
<div class="mw-collapsible-content"> | <div class="mw-collapsible-content"> | ||
Line 8: | Line 10: | ||
The electric field is a region around a charged particle or object within which a force would be exerted on other objects. | The electric field is a region around a charged particle or object within which a force would be exerted on other objects. | ||
If we put a charged particle at a location and it experiences a force, it would be logical to assume that there is something present that | If we put a charged particle at a location and it experiences a force, it would be logical to assume that there is something present that | ||
is interacting with the particle. This "virtual force" is in essence the electric field. | is interacting with the particle. This "virtual force" is, in essence, the electric field. | ||
===A Mathematical Model=== | ===A Mathematical Model=== | ||
Line 20: | Line 22: | ||
field. | field. | ||
You can also visualize the electric field lines using a simulator[http://www.flashphysics.org/electricField.html]. | |||
The net electric field at a location in space is the vector sum of the individual contributions from all the sources of electric field in that space. This uses the principle of superposition. | |||
Electric field is a expressed as a vector that tends towards negative charges and away from positive. | |||
==Coulomb and NonCoulomb Electric Fields== | |||
Commonly this topic refers to Coulomb Electric fields, which are produced from superposing individual radial fields from charges and explicitly defined regions of electric field. There exists a second kind called NonCoulomb electric fields that are produced from a varying magnetic field. These electric fields are similar to the pattern of magnetic field produced from a wire because they are both circular. NonCoulomb electric fields (<math>E_{NC}</math>) follow the curled right-hand-rule with the thumb pointing in the direction of <math> \frac{-dB}{dt} </math> and the fingers curl along the direction of <math>E_{NC}</math>. | |||
==Examples== | ==Examples== | ||
Line 44: | Line 54: | ||
D) The charges exert forces on each other equal in magnitude and pointing in the same direction. | D) The charges exert forces on each other equal in magnitude and pointing in the same direction. | ||
The answer is | The answer is C, which can be reasoned even by an extension of Newton's Third Law. Using the simple equation in this page, it is also possible to derive and reason this result. Notice that the forces are opposite in direction! The equations above relate vectors, an important concept in physics. | ||
Note: Just because the forces are equal does not mean that the accelerations, velocities, or motions of the charges are equal; these depend on both the initial velocities and the masses of both charges. | |||
===Difficult=== | ===Difficult=== | ||
The number of electric field lines passing through a unit cross sectional area is indicative of: | The number of electric field lines passing through a unit cross-sectional area is indicative of: | ||
A)field direction | A)field direction | ||
Line 59: | Line 71: | ||
E)rate of energy transfer | E)rate of energy transfer | ||
The answer is C | The answer is C since the number of electric field lines through an area is how field strength can be qualitatively and quantitatively determined. Field lines come out of positive charges and go into negative charges. | ||
Field strength can be inferred by placing a charge with known electric and mass properties and measuring the force exerted. In the absence of other external forces, this exerted force is a product of the charge and the electric field at that location. | |||
==Connectedness== | ==Connectedness== | ||
The electric field is made up. It's a lie. It's a concept that an English intellectual by the name of Michael Faraday made up centuries ago to think about the universe in a different way. But it this concept that is Faraday's greatest gift to the world. The electric field allows us to think about point charges, charge distributions, and current. It allows us to better understand electricity, a concept that would go on to spur some of the greatest inventions of the entire history of humankind. And now, with advances in areas like quantum computing and bioengineering where circuits are regularly employed to push the boundaries of science and engineering, we have Michael Faraday to thank. Devices that save lives or improve their quality, such as neuroprosthetics or pacemakers, rely on the principles theorized by Faraday long ago. Electric field is a useful visualization of a complex reality composed of interacting waves and interactions. The method of describing electric fields with vectors allowed for the Maxwell Equations to be derived, which drastically improved our understanding of electricity, magnetism, and how they are related. | |||
==History== | ==History== | ||
It was in 1831 that Hans Christian Oersted demonstrated that by applying an electric current through a wire, a magnetic field could be produced. How was this verified? The needle from a nearby compass was deflected accordingly. Michael Faraday would go on to demonstrate electromagnetic induction, in which Faraday resolved the issue of whether magnetism could produce electricity (which it could if the magnetic effect was set in motion, creating a resulting current). But it was not until 1864 that a Scottish physicist by the name of James Clerk Maxwell came along to provide a unifying statement for electromagnetism by way of his groundbreaking publication 'Dynamical Theory of the Electric Field'. Maxwell's equations were a set of four equations that expressed, mathematically, the behaviors in which electric and magnetic fields participated. | |||
== See also == | |||
===External links=== | |||
Interactive Electric Field [https://phet.colorado.edu/sims/charges-and-fields/charges-and-fields_en.html] | |||
Electric Field Simulator [http://www.flashphysics.org/electricField.html] | |||
==References== | |||
The following references were used while writing this page: | |||
http://www.rare-earth-magnets.com/history-of-magnetism-and-electricity | |||
https://en.wikipedia.org/wiki/Electric_field |
Latest revision as of 02:08, 23 November 2016
Electric field
Claimed by David Gamero (Fall 2016)
The electric field created by a charge is present throughout space at all times, whether or not there is another charge around to feel its effects. The electric field created by a charge penetrates through matter. The field permeates the neighboring space, biding its time until it can affect anything brought into its space of interaction.
The Main Idea
To be exact, the definition of the Electric Field is as follows:
The electric field is a region around a charged particle or object within which a force would be exerted on other objects.
If we put a charged particle at a location and it experiences a force, it would be logical to assume that there is something present that is interacting with the particle. This "virtual force" is, in essence, the electric field.
A Mathematical Model
The electric field can be expressed mathematically as follows:
[math]\displaystyle{ {\vec{F_{net}} = 0 \Leftrightarrow \frac{d\vec{v}}{dt}} = 0 }[/math]
[math]\displaystyle{ {\vec{F_{2}} = {q_{1}}{\vec{E_{1}}} \Leftrightarrow \frac{d\vec{v}}{dt}} }[/math]
which can be translated to postulate that the force on particle 2 is determined by the charge of particle 2 and the electric field.
You can also visualize the electric field lines using a simulator[1].
The net electric field at a location in space is the vector sum of the individual contributions from all the sources of electric field in that space. This uses the principle of superposition. Electric field is a expressed as a vector that tends towards negative charges and away from positive.
Coulomb and NonCoulomb Electric Fields
Commonly this topic refers to Coulomb Electric fields, which are produced from superposing individual radial fields from charges and explicitly defined regions of electric field. There exists a second kind called NonCoulomb electric fields that are produced from a varying magnetic field. These electric fields are similar to the pattern of magnetic field produced from a wire because they are both circular. NonCoulomb electric fields ([math]\displaystyle{ E_{NC} }[/math]) follow the curled right-hand-rule with the thumb pointing in the direction of [math]\displaystyle{ \frac{-dB}{dt} }[/math] and the fingers curl along the direction of [math]\displaystyle{ E_{NC} }[/math].
Examples
The following examples are to test your basic understanding of the Electric Field. For more examples that test your knowledge of all three of the laws, peruse the class textbook.
Simple
Which way is the electric field going for a negatively charged particle?
It's easy to see that the electric field is pointing toward the negatively charged particle. The electric field is tending toward the negatively charged particle.
Middling
Two charged objects are separated by a distance d. The first charge is larger in magnitude than the second charge:
A) The first charge exerts a larger force on the second charge.
B) The second charge exerts a larger force on the first charge.
C) The charges exert forces on each other that are equal in magnitude and opposite in direction.
D) The charges exert forces on each other equal in magnitude and pointing in the same direction.
The answer is C, which can be reasoned even by an extension of Newton's Third Law. Using the simple equation in this page, it is also possible to derive and reason this result. Notice that the forces are opposite in direction! The equations above relate vectors, an important concept in physics. Note: Just because the forces are equal does not mean that the accelerations, velocities, or motions of the charges are equal; these depend on both the initial velocities and the masses of both charges.
Difficult
The number of electric field lines passing through a unit cross-sectional area is indicative of:
A)field direction
B)charge density
C)field strength
D)charge motion
E)rate of energy transfer
The answer is C since the number of electric field lines through an area is how field strength can be qualitatively and quantitatively determined. Field lines come out of positive charges and go into negative charges. Field strength can be inferred by placing a charge with known electric and mass properties and measuring the force exerted. In the absence of other external forces, this exerted force is a product of the charge and the electric field at that location.
Connectedness
The electric field is made up. It's a lie. It's a concept that an English intellectual by the name of Michael Faraday made up centuries ago to think about the universe in a different way. But it this concept that is Faraday's greatest gift to the world. The electric field allows us to think about point charges, charge distributions, and current. It allows us to better understand electricity, a concept that would go on to spur some of the greatest inventions of the entire history of humankind. And now, with advances in areas like quantum computing and bioengineering where circuits are regularly employed to push the boundaries of science and engineering, we have Michael Faraday to thank. Devices that save lives or improve their quality, such as neuroprosthetics or pacemakers, rely on the principles theorized by Faraday long ago. Electric field is a useful visualization of a complex reality composed of interacting waves and interactions. The method of describing electric fields with vectors allowed for the Maxwell Equations to be derived, which drastically improved our understanding of electricity, magnetism, and how they are related.
History
It was in 1831 that Hans Christian Oersted demonstrated that by applying an electric current through a wire, a magnetic field could be produced. How was this verified? The needle from a nearby compass was deflected accordingly. Michael Faraday would go on to demonstrate electromagnetic induction, in which Faraday resolved the issue of whether magnetism could produce electricity (which it could if the magnetic effect was set in motion, creating a resulting current). But it was not until 1864 that a Scottish physicist by the name of James Clerk Maxwell came along to provide a unifying statement for electromagnetism by way of his groundbreaking publication 'Dynamical Theory of the Electric Field'. Maxwell's equations were a set of four equations that expressed, mathematically, the behaviors in which electric and magnetic fields participated.
See also
External links
Interactive Electric Field [2]
Electric Field Simulator [3]
References
The following references were used while writing this page:
http://www.rare-earth-magnets.com/history-of-magnetism-and-electricity